Warm-up Question:                   1
• What was the most confusing part of Monday’s
  lecture?
 A. The sign of shear stress
 B. Why do we need plane stress?
 C. Wait, what is plane stress?
 D. Mohr’s circle
 E. Principal stresses and max shear stress
                                                                                               7
http://www.gereports.com/post/112705004705/ge-develops-jet-engines-made-from-ceramic-matrix/
                                                                                        8
                                          http://www.mece.ualberta.ca/~wmoussa/lab/research.
                                                                 htm
http://galleryhip.com/tensile-test.html
                          Objectives                               9
• Use the condition of triaxial stress to determine the
    maxiumum shear stress from principle stresses
•   Define the condition of plane strain
•   Perform coordinate transformation of plane strain
•   Use Mohr’s circle to visualize coordinate transformations of
    strain and find the maximum shear strain
                             Mohr s circle                                  10
• Mohr s circle is a convenient way to visually remember the two-
    dimensional transformation equations.
•   Approach:
    1.Make 2D axes :
      • right = positive normal stress
      • down = positive shear stress
    2.Plot (σx, τxy) and (σy, −τxy) (remember sign convention for τ!)
    3.Draw a line between both points to be diameter of circle.
    4.Draw circle centered at midpoint of line.
    5.Rotate by points by 2θ, read off new (σx’, τx’y’) and (σy’, −τx’y’)
             Mohr’s circle resources                   11
• https://www.youtube.com/watch?v=-bIh3xSZBqE
• http://www.ijee.ie/OnlinePapers/Interactive/Philpot/mo
 hr_learning_tool.htm
                  Mohr s circle            12
                                  max normal
                                    stress
min normal
  stress          ave normal
                    stress
      max shear
       stress
Example   13
                         Question (14):                                      14
• Due to the applied loading, the element at point A on the solid shaft is
  subjected to the state of stress shown. Determine the principal stresses
  acting at this point.
  First: What is the stress state?
  A. σx = −12 ksi, σy = 0 ksi, τxy = +6 ksi
  B. σx = −12 ksi, σy = 0 ksi, τxy = −6 ksi
  C. σx = +12 ksi, σy = 0 ksi, τxy = +6 ksi
  D. σx = +12 ksi, σy = 0 ksi, τxy = −6 ksi
                         Question (15):                                      15
• Due to the applied loading, the element at point A on the solid shaft is
  subjected to the state of stress shown. Determine the principal stresses
  acting at this point.
  Next: Where is the center for Mohr s circle?
  A. (0 ksi, 0 ksi)
  B. (−6 ksi, 0 ksi)
  C. (−12 ksi, 0 ksi)
  D. (−6 ksi, −6 ksi)
  E. (−12 ksi, −6 ksi)
                         Question (16):                                      16
• Due to the applied loading, the element at point A on the solid shaft is
  subjected to the state of stress shown. Determine the principal stresses
  acting at this point.
  Next: What is the radius for Mohr s circle?
  A. 6.00 ksi
  B. 8.49 ksi
  C. 12.0 ksi
  D. 19.0 ksi
                         Question (17):                                      17
• Due to the applied loading, the element at point A on the solid shaft is
  subjected to the state of stress shown. Determine the principal stresses
  acting at this point.
  Finally: What are the principal stresses?
  A. −1.76 ksi, −10.2 ksi
  B. 0 ksi, −12.0 ksi
  C. 2.49 ksi, −14.5 ksi
  D. 11.9 ksi, −23.0 ksi
                              Example                                        18
• Due to the applied loading, the element at point A on the solid shaft is
  subjected to the state of stress shown. Determine the principal stresses
  acting at this point.
        Transformation of stress and strain   21
Plane stress
   Simplification of loading to a plane
   Sign convention
Transformation of coordinates
   Transforming loads and areas from one
   reference frame (coordinate axes) to
   another
Principal stresses and directions
   Eigenvalues and eigenvectors of stress
   Max/min normal stress
   Max shear stress
Mohr s circle
   geometric device to compute transform
Multiple loads in 3D
  principle stresses, max shear stress
Plane strain
  simplify a deformation to a single plane
Transformation of coordinates
  transforming displacements from one
  reference frame to another
                    General state of stress         22
• A general state of stress has 6 components:
  • 3 normal: σx σy σz
  • 3 shear: τyz τxz τxy
  • The components depend on the choice of
      coordinate system: xyz
•   For a different cube section, equilibrium can
    be applied to faces as before.
•   Principal stresses in 3D are defined the
    same as before:
    • Identify three ________________that
      have only ______________
    • Normal stress: σA is pointed along A
      (where A is the vector normal for a plane)
    • Principal stresses/planes =
      eigenvalue/eigenvectors for stress.
       Graphical stress tensor components            23
• Stress   area = force   Fi = Σj=xyz σij Aj
                   σxx=σx        σxy=τxy   σxz=τxz
                  σyx=τxy        σyy=σy    σyz=τyz
                   σzx=τxz       σzy=τyz   σzz=σz
                           Triaxial stress        24
• Principal stresses in 3D
  • Solutions to eigenvalue problem:
    • σA = sA
    • Three perpendicular A s each with own
        eigenvalue s
      • Sort eigenvalues (principal stresses):
        σmin ≤ σint ≤ σmax
•   For plane stress...
    • One principal stress is _____
      (perpendicular to plane)
    • Other two are principal stresses in plane
    • ______________ into σmin ≤ σint ≤ σmax
      depending on _____ of in-plane principal
      stresses
                      Maximum shear stress        25
  • Given three principal stresses
    σmin ≤ σint ≤ σmax
    we can find the maximum shear stresses in
    the three planes:
  1.min-int: τ = (σint − σmin)/2
  2.min-max: τ = (σmax − σmin)/2
  3.int-max: τ = (σmax − σint)/2
τ = (σint − σmin)/2
                            τ = (σmax − σint)/2
                      τ = (σmax − σmin)/2
       Maximum shear stress: plane stress                   26
• The same ideas apply for plane stress,
  where one principal stress is zero.
• Given three principal stresses
  σmin ≤ σint ≤ σmax
  we can find the maximum shear stresses in
  the three planes:
1.min-int: τ = (σint − σmin)/2
2.min-max: τ = (σmax − σmin)/2
3.int-max: τ = (σmax − σint)/2
           0 ≤ σ2 ≤ σ1                        σ2 ≤ 0 ≤ σ1
                              Question:                                         27
• The point on the surface of the cylindrical pressure vessel is subjected to
  a state of plane stress. Determine the absolute maximum shear stress at
  this point.
  First: What are the three principal
  stresses?
  A. −32 MPa, −16 MPa,        0 MPa
  B. −16 MPa,       0 MPa, +32 MPa
  C. −16 MPa, +8 MPa, +32 MPa
  D.     0 MPa, +16 MPa, +32 MPa
  E. +16 MPa, +24 MPa, +32 MPa
                              Question:                                         28
• The point on the surface of the cylindrical pressure vessel is subjected to
  a state of plane stress. Determine the absolute maximum shear stress at
  this point.
  Next: What is the absolute maximum
  shear stress?
  A.    0 MPa
  B.    8 MPa
  C. 16 MPa
  D. 24 MPa
  E. 32 MPa
                              Question:                                         29
• The point on the surface of the cylindrical pressure vessel is subjected to
  a state of plane stress. Determine the absolute maximum shear stress at
  this point.
  Finally: What is the maximum
  shear stress in the plane of loading?
  A.    0 MPa
  B.    8 MPa
  C. 16 MPa
  D. 24 MPa
  E. 32 MPa
                               Example                                          30
• The point on the surface of the cylindrical pressure vessel is subjected to
  a state of plane stress. Determine the absolute maximum shear stress at
  this point.
                             Plane strain                                         37
• A general state of strain has 6 components:
  • 3 normal: ϵx ϵy ϵz
  • 3 shear: γyz γxz γxy
  • The components depend on the choice of
      coordinate system: xyz
•   There may be a plane which contains the
    only nonzero strain components
    • E.g., all deformations contained in a plane
    • Choose the xy coordinate system to
      contain the nonzero strains
    • 2 normal: ϵx ϵy
    • 1 shear: γxy
•   The components depend on the choice of
    coordinate system: xy
•   Note: ____________ ≠ _____________
    • Due to Poisson effect (next week!):
      normal stresses in xy plane create
      normal strains in z direction, too.
                                                    plane stress ≠ plane strain
                  Transforming plane strain                                          38
• A state of plane strain has three components
  • The components are _______________ of the
      ________________________ making it into a parallelogram
    • ϵx, ϵy, γxy all depend on how that square is oriented.
    • The components for one choice can be determined from the
      components for another choice by constructing ________, and taking
      ___________.
•   Remember the definitions of strain: change in a vector
    • ϵx = change of i in direction of i
    • ϵy = change of j in direction of j
    • γxy = half change of i in direction of j, half change of j in direction of i
    before              after
    strain              strain
       Graphical strain tensor components                  39
• Strain   length = length change   δℓi = Σj=xyz εij ℓj
                   εxx=ϵx           εxy=½γxy εxz=½γxz
                 εyx=½γxy            εyy=ϵy    εyz=½γyz
                 εzx=½γxz           εzy=½γyz      εzz=ϵz
                Transforming plane strain                                          40
• Remember the definitions of strain: change in a vector
  • ϵx = change of i in direction of i
  • ϵy = change of j in direction of j
  • γxy = half change of i in direction of j, half change of j in direction of i
• Consider ϵx : change of i in direction of i
                Transforming plane strain                                          41
• Remember the definitions of strain: change in a vector
  • ϵx = change of i in direction of i
  • ϵy = change of j in direction of j
  • γxy = half change of i in direction of j, half change of j in direction of i
• Consider ϵx : change of i in direction of i
dot product
  with i’
                Transforming plane strain                                          42
• Remember the definitions of strain: change in a vector
  • ϵx = change of i in direction of i
  • ϵy = change of j in direction of j
  • γxy = half change of i in direction of j, half change of j in direction of i
• Consider γx y : change of i in direction of j
dot product
  with j’
                Transforming plane strain                                          44
• Remember the definitions of strain: change in a vector
  • ϵx = change of i in direction of i
  • ϵy = change of j in direction of j
  • γxy = half change of i in direction of j, half change of j in direction of i
• Consider ϵy : change of j in direction of j
                Transforming plane strain                                          46
• Remember the definitions of strain: change in a vector
  • ϵx = change of i in direction of i
  • ϵy = change of j in direction of j
  • γxy = half change of i in direction of j, half change of j in direction of i
• Consider ϵy : change of j in direction of j
dot product
  with j’
      Transforming plane strain: summary                                   48
• Transforming strain is the same as for stress: σ→ϵ, τ→½γ
• We can simplify the expressions by using double-angle formulae
  • sin 2θ = 2 sin θ cos θ
  • cos 2θ = cos2θ − sin2θ
• Note: ϵx + ϵy = ϵx + ϵy
• Note the similarity in equations—what we did for stress, we do for strain:
  • Same special cases: 180 , 90 , 45 rotations
  • Mohr s circle to rotate in plane
  • Principal strains (max/min normal strain)                =
  • Max shear strain
  • Be mindful of the 1/2 factor for shear in Mohr s circle!
                              Question:                                      49
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
  equivalent strains acting on an element of material oriented at the point
  clockwise 30 from the original position.
  First: What is the average normal strain?
  A. +400(10−6)
  B. +200(10−6)
  C. +100(10−6)
  D. −100(10−6)
  E. −200(10−6)
                              Question:                                      50
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
  equivalent strains acting on an element of material oriented at the point
  clockwise 30 from the original position.
  Next: What are cos 2θ and sin 2θ?
  A. cos 2θ=+√3/2, sin 2θ=+1/2
  B. cos 2θ=+1/2, sin 2θ=+√3/2
  C. cos 2θ=+√3/2, sin 2θ=−1/2
  D. cos 2θ=+1/2, sin 2θ=−√3/2
                              Question:                                      51
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
  equivalent strains acting on an element of material oriented at the point
  clockwise 30 from the original position.
  Next: What is ϵx ?
  A. +386(10−6)
  B. +213(10−6)
  C. −13.4(10−6)
  D. −186(10−6)
                              Question:                                      52
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
  equivalent strains acting on an element of material oriented at the point
  clockwise 30 from the original position.
  Next: What is ϵy ?
  A. +386(10−6)
  B. +213(10−6)
  C. −13.4(10−6)
  D. −186(10−6)
                              Question:                                      53
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
  equivalent strains acting on an element of material oriented at the point
  clockwise 30 from the original position.
  Finally: What is γx y ?
  A. +793(10−6)
  B. +396(10−6)
  C. −296(10−6)
  D. −592(10−6)
                                 Example                                       54
  • A differential element of material at a point is subjected to a state of
    plane strain ϵx=500(10−6), ϵy=−300(10−6), γxy=200(10−6). Determine the
    equivalent strains acting on an element of material oriented at the point
    clockwise 30 from the original position.
                            +793(10−6) / 2
−13.4(10−6)
                                     +793(10−6) / 2
          +213(10−6)
                         Principal strains                                56
• The magnitude of normal and shear strains depends on orientation of
    section with respect to the deformation
•   From a given plane strain, we can find the angle that produces an
    extremum in normal strain (max or min):
• Produces two solutions: θp1 and θp2, which are 90 apart (max and min)
• Finding the max and min normal stresses by substituting θp1 or θp2:
• Orientation for max shear strain found similarly:
• In that coordinate system:
                         Principal strains                                     57
• Principal strains are the __________________________normal strains.
• The ______ on which these act are the principal _____________.
• Note: if a material has ___________ mechanical response then the
    principal directions are the _____________ for the principal planes.
    • This is because in an isotropic material, normal stresses only produce
      normal strains, never shear strains.
•   The principal directions experience no shear strain
    • Using the principal directions as coordinate axes, there are no off-
      diagonal components to the strain matrix.
    • The strain tensor is diagonal, which makes the principal strains the
      eigenvalues of the strain tensor, and the principal directions the
      eigenvectors of the strain tensor.
                   Mohr s circle for strain                               58
• Mohr s circle is a convenient way to visually remember the two-
    dimensional transformation equations.
•   Approach:
    1.Make 2D axes :
      • right = positive normal strain
      • down = positive shear strain divided by 2
    2.Plot (ϵx, ½γxy) and (ϵy, −½γxy) (remember sign convention for γ/2!)
    3.Draw a line between both points to be diameter of circle.
    4.Draw circle centered at midpoint of line.
    5.Rotate by points by 2θ, read off new (ϵx’, ½γx’y’) and (ϵy’, −½γx’y’)
        Mohr s circle for strain                   59
                         ave normal   max normal
                           strain       strain
min normal
  strain
             max shear
              strain/2
                              Question:                                         60
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
  First: What is the average normal strain?
  A. −75.0(10−6)
  B. −150(10−6)
  C. −275(10−6)
  D. −550(10−6)
                              Question:                                         61
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
  Next: What is the radius of Mohr s circle?
  A. 85.0(10−6)
  B. 110(10−6)
  C. 278(10−6)
  D. 286(10−6)
                              Question:                                         62
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
  Next: What are the principal strains?
  A. −353(10−6), +203(10−6)
  B. −203(10−6), +353(10−6)
  C. −214(10−6), +64.0(10−6)
  D. −64.0(10−6), +214(10−6)
                              Question:                                         63
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
  Next: What are the principal directions
  relative to x?
  A. −85.9 and +4.14
  B. −8.28 and +172
  C. −4.14 and +85.9
  D. −172 and +8.28
                              Question:                                         64
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
  Finally: What is the maximum shear strain?
  A. 85.0(10−6)
  B. 110(10−6)
  C. 278(10−6)
  D. 286(10−6)
  E. 556(10−6)
                               Example                                          65
• A differential element of material at a point is subjected to a state of
  plane strain ϵx=−350(10−6), ϵy=200(10−6), γxy=80(10−6). Determine the
  principal strains at the point and the orientation of principal directions.
                         +203(10−6)
     −353(10−6)
                              Summary                                          67
• Used the condition of triaxial stress to determine the maxiumum shear
    stress from principle stresses
•   Defined the condition of plane strain
•   Performed coordinate transformation of plane strain
•   Used Mohr’s circle to visualize coordinate transformations of strain and
    find the maximum shear strain